Method of designing equal conic intraocular lens
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[0012] Given that the B-IOL must have symmetric surfaces (design requirement) and the paraxial power of the lens is the labeled power, the only true design parameter is the conic coefficient K. It is possible to set the conic constant so that the marginal ray (which just clears the edge of the clear aperture of the lens) for a distant object intersects the paraxial focus. The distance between the intersection of the off-axis ray with the optical axis and the paraxial focus is called the longitudinal aberration of the ray. For the case of zero longitudinal aberration at the marginal ray, the longitudinal aberration across the semi-diameter is graphed in FIG. 1.A. Note that in FIG. 1.A, the aberration at ray height of zero (the chief ray) is zero as is the ray at the edge of the lens. To reduce the overall sum of the longitudinal aberration, we can alternatively select the conic coefficient so that a ray at a height equal to 0.7071 of the clear aperture radius intersects the paraxial ...
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